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Nuclear level densities and \(\gamma\)-ray strength functions of \(^{87}\mathrm{Kr}\) -- First application of the Oslo Method in inverse kinematics

The \(\gamma\)-ray strength function (\(\gamma\)SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo Method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton...

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Published in:arXiv.org 2019-11
Main Authors: Ingeberg, V W, Siem, S, Wiedeking, M, Sieja, K, Bleuel, D L, Brits, C P, Bucher, T D, Dinoko, T S, Easton, J L, Görgen, A, Guttormsen, M, Jones, P, Kheswa, B V, Khumalo, N A, Larsen, A C, Lawrie, E A, Lawrie, J J, Majola, S N T, Malatji, K L, Makhathini, L, Maqabuka, B, Negi, D, Noncolela, S P, Papka, P, Sahin, E, Schwengner, R, Tveten, G M, Zeiser, F, Zikhali, B R
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Language:English
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Summary:The \(\gamma\)-ray strength function (\(\gamma\)SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo Method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton-\(\gamma\) coincidence events from the \(\mathrm{d}(^{86}\mathrm{Kr}, \mathrm{p}\gamma)^{87}\mathrm{Kr}\) reaction were measured at iThemba LABS and the \(\gamma\)SF and NLD in \(^{87}\mathrm{Kr}\) obtained. The low-energy region of the \(\gamma\)SF is compared to Shell Model calculations which suggest this region to be dominated by M1 strength. The \(\gamma\)SF and NLD are used as input parameters to Hauser-Feshbach calculations to constrain \((\mathrm{n},\gamma)\) cross sections of nuclei using the TALYS reaction code. These results are compared to \(^{86}\mathrm{Kr}(n,\gamma)\) data from direct measurements.
ISSN:2331-8422
DOI:10.48550/arxiv.1806.09991